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RIAA Preamps Part 2 - Tube CAD Journal

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+210V<br />

5.5k<br />

8k<br />

11k<br />

+100V<br />

.0099µF<br />

+130V<br />

117k<br />

+130V<br />

.47µF<br />

300 32.5k<br />

6DJ8 +2V 6DJ8 +2V<br />

300<br />

.03µF<br />

6DJ8 +24V<br />

.1µF 300<br />

6DJ8 +2V<br />

1M<br />

47k<br />

200<br />

200<br />

8.7k<br />

24k<br />

1M<br />

200<br />

Cascading these two functions results in the<br />

same curve as the traditional two function<br />

combination creates. So, why bother with this<br />

alternate approach Beyond the mental<br />

stretching, which is always for the good, this<br />

alternative approach engenders new phono<br />

preamp topologies, with some interesting<br />

benefits and one negative. The first benefit is<br />

that the 50Hz low-pass filter can filter more<br />

power supply noise away from the output signal<br />

than the 2122Hz can.<br />

.1µF<br />

1M<br />

+10V<br />

200<br />

47k<br />

Ra<br />

1200<br />

10k<br />

91k<br />

R1<br />

C1<br />

+12V<br />

C2<br />

Rk<br />

.266µF<br />

+210V<br />

.0318µF<br />

A single-triode phono preamp<br />

Second, the 500Hz to 2122Hz shelving<br />

network can be implemented within one<br />

grounded–cathode amplifier, i.e. a single triode<br />

<strong>RIAA</strong> equalized preamp. Usually a cathode<br />

resistor is bypassed with a large valued<br />

capacitor, so as to ensure adequate lowfrequency<br />

response. But if the bypass capacitor’s<br />

value is reduced greatly, it introduces a shelving<br />

function, wherein the high-frequency gain is<br />

greater than the low-frequency gain, with the<br />

ratio being equal to the bypassed gain over the<br />

unbypassed gain or<br />

1 .<br />

Ratio = 1 + (mu + 1)R k<br />

R a + r p<br />

The transition frequencies are based on the<br />

capacitor’s value and the time constants it forms<br />

with the triode’s r p and its plate and cathode<br />

resistor values:<br />

R k C k = 75µS<br />

[(R a + r p )/(mu + 1) || R k ]C k = 318µS<br />

Of course, one triode is not going to provide<br />

enough gain in most cases, so additional gain<br />

stages will be needed.<br />

The overarching liability of this different<br />

path to <strong>RIAA</strong> equalization is the –12dB insertion<br />

loss beyond the expected losses, which brings it<br />

1kHz insertion loss down to –32dB. With this<br />

equalization network, the near DC and subsonic<br />

frequencies are reduced by –12dB, whereas the<br />

traditional path retained all of the gain at the<br />

bottom of range. Now, -12dB is just too much to<br />

pay in most two-gain-stage phono preamps, but<br />

it is almost nothing in a three-gain-stage preamp,<br />

where the problem is usually having too much<br />

gain. Still the advantage of using a portion of the<br />

equalization network in double duty either, as a<br />

pseudo coupling capacitor or a partial cathodebypass<br />

capacitor, is tempting.<br />

< PREVIOUS Pg. 13<br />

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